A zoom lens system comprising a first lens unit of negative power, a second lens unit of positive power and a third lens unit of positive power, wherein in zooming, the lens units move respectively along an optical axis so that an interval of first lens unit and second lens unit decreases while an interval of second lens unit and third lens unit changes with variable magnification, the first lens unit comprises one object side negative lens element and one image side positive lens element, which have an aspheric surface, and the conditions: n12>1. 88, v12<26 and 5.0<αiW<20.0 (ωW>30, n12 and v12 are refractive index and abbe number, respectively, of the image side positive lens element of the first lens unit, αi W is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit) are satisfied.
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1. A zoom lens system for forming an optical image of an object with a variable magnification, in order from the object side to the image side, comprising:
a first lens unit having negative optical power; a second lens unit having positive optical power; and a third lens unit having positive optical power, wherein
in zooming from a wide-angle limit to a telephoto limit, the lens units move respectively along an optical axis in such a manner that an interval between the first lens unit and the second lens unit decreases while an interval between the second lens unit and the third lens unit changes so that the variable magnification is achieved,
the first lens unit comprises: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side that is arranged with an air space on the image side of the object side negative lens element,
each of the two lens elements constituting the first lens unit has an aspheric surface, and
the following conditions (1), (2) and (3) are satisfied:
n12>1.88 (1) v12<26 (2) 5.0<αiW<20.0 (3) (where, ωW≧33.97)
in which,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
13. A camera capable of shooting a photographic object and then outputting its image as an electric image signal, comprising:
an imaging device including a zoom lens system that forms the optical image of the photographic object with a variable magnification, and an image sensor that converts the optical image of the photographic object formed by the zoom lens system into the electric image signal, wherein
the zoom lens system, in order from the object side serving as the photographic object side to the image side, comprises: a first lens unit having negative optical power; a second lens unit having positive optical power; and a third lens unit having positive optical power,
in zooming from a wide-angle limit to a telephoto limit, the lens units move respectively along an optical axis in such a manner that an interval between the first lens unit and the second lens unit decreases while an interval between the second lens unit and the third lens unit changes so that the variable magnification is achieved,
the first lens unit comprises: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side that is arranged with an air space on the image side of the object side negative lens element,
each of the two lens elements constituting the first lens unit has an aspheric surface, and
the following conditions (1), (2) and (3) are satisfied:
n12>1.88 (1) v12<26 (2) 5.0<αiW<20.0 (3) (where, ωW≧33.97)
in which,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
7. An imaging device capable of converting an optical image of a photographic object into an electric image signal and then outputting the signal, comprising:
a zoom lens system that forms the optical image of the photographic object with a variable magnification; and
an image sensor that converts the optical image of the photographic object formed by the zoom lens system into the electric image signal, wherein
the zoom lens system, in order from the object side serving as the photographic object side to the image side, comprises: a first lens unit having negative optical power; a second lens unit having positive optical power; and a third lens unit having positive optical power,
in zooming from a wide-angle limit to a telephoto limit, the lens units move respectively along an optical axis in such a manner that an interval between the first lens unit and the second lens unit decreases while an interval between the second lens unit and the third lens unit changes so that the variable magnification is achieved,
the first lens unit comprises: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side that is arranged with an air space on the image side of the object side negative lens element,
each of the two lens elements constituting the first lens unit has an aspheric surface, and
the following conditions (1), (2) and (3) are satisfied:
n12>1.88 (1) v12<26 (2) 5.0<αiW<20.0 (3) (where, ωW≧33.97) in which,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
2. The zoom lens system as claimed in
n11>1.50 (4) v11>35 (5) n12−n11>0.10 (6) v11−v12>15.0 (7) wherein,
n11 is a refractive index of the object side negative lens element of the first lens unit,
v11 is an abbe number of the object side negative lens element of the first lens unit,
n12 is the refractive index of the image side positive lens element of the first lens unit, and
v12 is the abbe number of the image side positive lens element of the first lens unit.
3. The zoom lens system as claimed in
T1/Y<1.5 (8) wherein,
T1 is a center thickness of the first lens unit, and
Y is the maximum image height.
4. The zoom lens system as claimed in
(T1+T2+T3)/Y<3.5 (9) wherein,
T1 is a center thickness of the first lens unit,
T2 is a center thickness of the second lens unit,
T3 is a center thickness of the third lens unit, and
Y is the maximum image height.
5. The zoom lens system as claimed in
6. The zoom lens system as claimed in
an object side surface of the most object side lens element that constitutes the second lens unit is aspheric, and wherein
the second lens unit, in order from the object side to the image side, comprises one set of positive cemented lens element and one positive lens element, or alternatively comprises one positive lens element, one set of cemented lens element and one positive lens element, or alternatively comprises two sets of positive cemented lens elements.
8. The imaging device as claimed in
n11>1.50 (4) v11>35 (5) n12−n11>0.10 (6) v11−v12>15.0 (7) wherein,
n11 is a refractive index of the object side negative lens element of the first lens unit,
v11 is an abbe number of the object side negative lens element of the first lens unit,
n12 is the refractive index of the image side positive lens element of the first lens unit, and
v12 is the abbe number of the image side positive lens element of the first lens unit.
9. The imaging device as claimed in
T1/Y<1.5 (8) wherein,
T1 is a center thickness of the first lens unit, and
Y is the maximum image height.
10. The imaging device as claimed in
(T1+T2+T3)/Y<3.5 (9) wherein,
T1 is a center thickness of the first lens unit,
T2 is a center thickness of the second lens unit,
T3 is a center thickness of the third lens unit, and
Y is the maximum image height.
11. The imaging device as claimed in
12. The imaging device as claimed in
an object side surface of the most object side lens element that constitutes the second lens unit of the zoom lens system is aspheric, and wherein
the second lens unit, in order from the object side to the image side, comprises one set of positive cemented lens element and one positive lens element, or alternatively comprises one positive lens element, one set of cemented lens element and one positive lens element, or alternatively comprises two sets of positive cemented lens elements.
14. The camera as claimed in
15. The camera as claimed in
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This application is based on application No. 2006-64711 filed in Japan on Mar. 9, 2006, the content of which is hereby incorporated by reference.
1. Technical Field
The present invention relates to a zoom lens system, an imaging device and a camera. In particular, the present invention relates to: a zoom lens system that has a high resolution, sufficient periphery illuminance ensured in the entire variable magnification range and high capability of compensating curvature of field, and that still has a short overall optical length at the time of non-use; an imaging device employing this zoom lens system; and a camera employing this imaging device.
2. Description of the Background Art
In the prior art, a large number of optical instruments have been developed that form an image of a photographic object onto an image sensor through a lens and then acquire the object image as an image. Recently, products such as digital still cameras and digital video cameras are spreading. Then, with the increase in the number of users, desire on these products is also growing. Among various types of these products, optical instruments having a zoom ratio of approximately three are comparatively small and still have an optical zoom function. Thus, these types are spreading remarkably widely as digital cameras of compact type or stylish type.
In the digital cameras of compact type, for the purpose of the property of easy carrying, further size reduction of the instruments is desired. In order to achieve the further size reduction of the digital cameras, the lens arrangement need be adopted such that the overall optical length (the distance measured from the top of the most object side lens surface of the entire lens system to the image surface) at the time of non-use should be reduced while lens elements that extend out relative to the main body by means of a multi-stage lens barrel at the time of use could be accommodated into the main body.
Meanwhile, as zoom lens systems suitable for digital still cameras of compact type, a large number of zoom lens systems of three-unit construction have been proposed that, for example, in order from the object side to the image side, comprise a first lens unit having negative optical power, a second lens unit having positive optical power, and a third lens unit having positive optical power.
In such a zoom lens system of three-unit construction, in zooming (magnification change) from a wide-angle limit to a telephoto limit, the air space between the first lens unit and the second lens unit decreases monotonically, while the air space between the second lens unit and the third lens unit varies, and while the third lens unit is fixed or moved.
Focus adjustment in the zoom lens system of three-unit construction is performed by moving the first lens unit or the third lens unit in the optical axis direction. In particular, from the perspective of size reduction of the entire optical instrument, in many cases, the focus adjustment is performed using the third lens unit which is less heavy, so that focusing onto the photographic object is achieved ranging from the infinity to a short distance. In contrast, when the focus adjustment is performed using the first lens unit, the first lens unit is larger than the third lens unit and hence requires a large size motor. This causes a tendency of size increase in the entire optical instrument.
The third lens unit having positive optical power has the effects of compensating curvature of field and bringing into a telecentric state the incident light onto a light receiving surface of the image sensor. Further, in many cases, the third lens unit is constructed from one or two lens elements having a small outer diameter, and hence can be driven at a high speed using a small size motor. Thus, when the third lens unit is adopted as a lens unit for focus adjustment, an optical instrument is realized that has a reduced size and permits rapid focusing.
The first lens unit and the second lens unit move in parallel to the optical axis along a cam groove formed in a cylindrical cam. In the cam groove, a groove for zooming and a groove for the time of non-use are connected to each other. The groove for the time of non-use reduces the interval between the lens units and moves all the three lens units to the image sensor side. This configuration reduces the overall optical length at the time of non-use. In this case, if the thickness of each lens unit could be reduced, the overall optical length at the time of non-use would be reduced further.
As such, in the prior art, design has been performed such that the zoom lens system should have the above configuration where the size is reduced in the part relevant to focus adjustment and in the entire lens system at the time of non-use, so that the overall optical length of the digital still camera has been reduced.
For example, Japanese Laid-Open Patent Publication No. 2005-134746 discloses a three-unit zoom lens, in order from the object side to the image side, comprising: a first lens unit having negative optical power that is composed of a negative-powered lens having an aspheric surface and a positive-powered lens; a second lens unit having positive optical power; and a third lens unit having positive optical power. In this three-unit zoom lens, the most object side negative-powered lens of the first lens unit is provided with a high refractive index, so that the lens thickness in the periphery part is reduced in a state that curvature of field at a wide-angle limit is compensated. This reduces the thickness of the entire first lens unit and hence the size of the optical system.
Further, for example, Japanese Laid-Open Patent Publication No. 2005-084597 discloses a three-unit zoom lens that, in order from the object side to the image side, comprises a first lens unit having negative optical power, a second lens unit having positive optical power and provided with a diaphragm, and a third lens unit having positive optical power, wherein in magnification change, the first lens unit moves relatively in a direction approaching to the second lens unit, while the second lens unit monotonically moves to the object side, and while the third lens unit moves to the object side and then moves reverse to the image side, and wherein when the object distance is infinity, the position of the third lens unit at a wide-angle limit is located on the object side relative to the position at a telephoto limit. In this three-unit zoom lens, a condition is set forth concerning the focal length of the first lens unit in such a manner that the compensation of curvature of field and the size reduction of the optical system can be achieved simultaneously.
Further, new optical materials having refractive indices or Abbe numbers in the range unavailable in the past can recently be obtained comparatively easily. Thus, proposals have been made that such optical materials are applied to the lenses included in a zoom lens so that size reduction may be achieved in the optical system.
For example, Japanese Laid-Open Patent Publication No. 2006-011096 discloses a zoom lens, in order from the object side to the image side, comprising: a first lens unit having negative optical power that is composed of a negative-powered lens having an aspheric surface and a positive-powered lens; a second lens unit having positive optical power; and a third lens unit having positive optical power, wherein the first lens unit includes a lens element having a refractive index exceeding 1.9.
Nevertheless, in the configuration of the three-unit zoom lens disclosed in Japanese Laid-Open Patent Publication No. 2005-134746, the positive-powered lens on the image side of the first lens unit has a low refractive index and still is a spherical lens. This causes a problem of insufficiency in the compensation of curvature of field.
Further, in the configuration of the three-unit zoom lens disclosed in Japanese Laid-Open Patent Publication No. 2005-084597, for the purpose of size reduction, the focal length of the first lens unit is set up rather short. Nevertheless, in this case, although the diameter of the lens can be constructed comparatively small, when the first lens unit is composed of two lenses, the optical power becomes excessive in the object side lens. Further, the thickness of the image side lens also increases for the purpose of compensation of chromatic aberration. This causes a problem of increase in the overall optical length at the time of non-use.
Further, the configuration of the zoom lens disclosed in Japanese Laid-Open Patent Publication No. 2006-011096 has a problem that the incident angle of light that is incident on the image sensor is excessively large especially at a wide-angle limit When the incident angle becomes large as described here, a loss is caused in the amount of light depending on shading characteristic of the image sensor, and thereby reduces the amount of periphery light in the shot image. Further, in the configuration of the zoom lens disclosed in Japanese Laid-Open Patent Publication No. 2006-011096, fluctuation in the incident angle at the time of zooming is also large. This causes a problem of large fluctuation in the seeing condition of the image in the periphery part.
An object of the present invention is to provide: a zoom lens system that has a high resolution, sufficient periphery illuminance ensured in the entire variable magnification range and high capability of compensating curvature of field, and that still has a short overall optical length at the time of non-use; an imaging device employing this zoom lens system; and a camera employing this imaging device.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the conventional art, and herein is disclosed:
a zoom lens system for forming an optical image of an object with a variable magnification, in order from the object side to the image side, comprising: a first lens unit having negative optical power; a second lens unit having positive optical power; and a third lens unit having positive optical power, wherein
in zooming from a wide-angle limit to a telephoto limit, the lens units move respectively along an optical axis in such a manner that an interval between the first lens unit and the second lens unit decreases while an interval between the second lens unit and the third lens unit changes so that the variable magnification is achieved,
the first lens unit comprises: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side that is arranged with an air space on the image side of the object side negative lens element,
each of the two lens elements constituting the first lens unit has an aspheric surface, and
the following conditions (1), (2) and (3) are satisfied:
n12>1.88 (1)
v12<26 (2)
5.0<αiW<20.0 (3)
(here, ωW>3)
where,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an Abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the conventional art, and herein is disclosed:
an imaging device capable of converting an optical image of a photographic object into an electric image signal and then outputting the signal, comprising:
a zoom lens system that forms the optical image of the photographic object with a variable magnification; and
an image sensor that converts the optical image of the photographic object formed by the zoom lens system into the electric image signal, wherein
the zoom lens system, in order from the object side serving as the photographic object side to the image side, comprises: a first lens unit having negative optical power; a second lens unit having positive optical power; and a third lens unit having positive optical power,
in zooming from a wide-angle limit to a telephoto limit, the lens units move respectively along an optical axis in such a manner that an interval between the first lens unit and the second lens unit decreases while an interval between the second lens unit and the third lens unit changes so that the variable magnification is achieved,
the first lens unit comprises: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side that is arranged with an air space on the image side of the object side negative lens element,
each of the two lens elements constituting the first lens unit has an aspheric surface, and
the following conditions (1), (2) and (3) are satisfied:
n12>1.88 (1)
v12<26 (2)
5.0<αiW<20.0 (3)
(here, ωW>30)
where,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an Abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the conventional art, and herein is disclosed:
a camera capable of shooting a photographic object and then outputting its image as an electric image signal, comprising:
an imaging device including a zoom lens system that forms the optical image of the photographic object with a variable magnification, and an image sensor that converts the optical image of the photographic object formed by the zoom lens system into the electric image signal, wherein
the zoom lens system, in order from the object side serving as the photographic object side to the image side, comprises: a first lens unit having negative optical power; a second lens unit having positive optical power; and a third lens unit having positive optical power,
in zooming from a wide-angle limit to a telephoto limit, the lens units move respectively along an optical axis in such a manner that an interval between the first lens unit and the second lens unit decreases while an interval between the second lens unit and the third lens unit changes so that the variable magnification is achieved,
the first lens unit comprises: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side that is arranged with an air space on the image side of the object side negative lens element,
each of the two lens elements constituting the first lens unit has an aspheric surface, and
the following conditions (1) and (2) are satisfied:
n12>1.88 (1)
v12<26 (2)
5.0<αiW<20.0 (3)
(here, ωW>30)
where,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an Abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
The present invention provides: a zoom lens system that has a high resolution, sufficient periphery illuminance ensured in the entire variable magnification range and capability of satisfactory compensation of curvature of field, and that still has a reduced thickness of the first lens unit and a short overall optical length at the time of non-use; and an imaging device employing this zoom lens system. The present invention further provides a small and high performance camera employing this imaging device.
This and other objects and features of this invention will become clear from the following description, taken in conjunction with the preferred embodiments with reference to the accompanied drawings in which:
Each zoom lens system according to Embodiments 1 to 5, in order from the object side to the image side, comprises: a first lens unit G1 having negative optical power; a diaphragm A; a second lens unit G2 having positive optical power; and a third lens unit G3 having positive optical power. In the zoom lens system according to Embodiments 1 to 5, in zooming from the wide-angle limit to the telephoto limit, the first lens unit G1 moves with locus of a convex to the image side, while the second lens unit G2 and the diaphragm A monotonically move to the object side, and while the third lens unit G3 moves with changing the interval with the second lens unit G2. That is, in the zoom lens system according to Embodiments 1 to 5, in zooming from the wide-angle limit to the telephoto limit, the lens units move respectively along the optical axis in such a manner that the interval between the first lens unit G1 and the second lens unit G2 decreases while the interval between the second lens unit G2 and the third lens unit G3 changes. Further, in each of
As shown in
Further, in the zoom lens system according to Embodiment 1, the second lens unit G2, in order from the object side to the image side, comprises: a positive meniscus third lens element L3 with the convex surface facing the object side; a negative meniscus fourth lens element L4 with the convex surface facing the object side; a negative meniscus fifth lens element L5 with the convex surface facing the object side; and a bi-convex sixth lens element L6. Among these, the third lens element L3 and the fourth lens element L4 are cemented with each other and thereby constitute a positive cemented lens element, while the fifth lens element L5 and the sixth lens element L6 are cemented with each other and thereby constitute a positive cemented lens element. Further, the third lens element L3 serving as the most object side lens element of the second lens unit G2 has an aspheric object side surface.
Further, in the zoom lens system according to Embodiment 1, the third lens unit G3 comprises solely a positive meniscus seventh lens element L7 with the convex surface facing the image side. The seventh lens element L7 has an aspheric image side surface.
In the zoom lens system according to Embodiment 1, as shown in Table 16 described later, the image side positive lens element L2 constituting the first lens unit G1 has a notably high refractive index. Thus, in the object side negative lens element L1, the thickness at large light beam height is easily ensured, so that the lens thickness can be reduced. Thus, in the zoom lens system according to Embodiment 1, the overall optical length at the time of non-use is reduced.
As shown in
In the zoom lens system according to Embodiment 2, the second lens unit G2, in order from the object side to the image side, comprises: a positive meniscus third lens element L3 with the convex surface facing the object side; a positive meniscus fourth lens element L4 with the convex surface facing the object side; a negative meniscus fifth lens element L5 with the convex surface facing the object side; and a bi-convex sixth lens element L6. Among these, the fourth lens element L4 and the fifth lens element L5 are cemented with each other and thereby constitute a cemented lens element. Further, the third lens element L3 serving as the most object side lens element of the second lens unit G2 has an aspheric object side surface.
In the zoom lens system according to Embodiment 2, the third lens unit G3 comprises solely a bi-convex seventh lens element L7. The seventh lens element L7 has an aspheric image side surface.
In the zoom lens system according to Embodiment 2, as shown in Table 16 described later, the image side positive lens element L2 constituting the first lens unit G1 has a comparatively high refractive index. Thus, edge thickness is relatively easily ensured even if the lens center thickness is reduced, so that the lens thickness can be reduced. Thus, in the zoom lens system according to Embodiment 2, the overall optical length at the time of non-use is reduced.
As shown in
Further, in the zoom lens system according to Embodiment 3, the second lens unit G2, in order from the object side to the image side, comprises: a positive meniscus third lens element L3 with the convex surface facing the object side; a negative meniscus fourth lens element L4 with the convex surface facing the object side; a negative meniscus fifth lens element L5 with the convex surface facing the object side; and a bi-convex sixth lens element L6. Among these, the third lens element L3 and the fourth lens element L4 are cemented with each other and thereby constitute a positive cemented lens element, while the fifth lens element L5 and the sixth lens element L6 are cemented with each other and thereby constitute a positive cemented lens element. Further, the third lens element L3 serving as the most object side lens element of the second lens unit G2 has an aspheric object side surface.
Further, in the zoom lens system according to Embodiment 3, the third lens unit G3 comprises solely a positive meniscus seventh lens element L7 with the convex surface facing the image side. The seventh lens element L7 has an aspheric image side surface.
In the zoom lens system according to Embodiment 3, as shown in Table 16 described later, the object side negative lens element L1 constituting the first lens unit G1 has a low refractive index, while the thickness at large light beam height is small. However, the image side positive lens element L2 of the first lens unit G1 has a comparatively high refractive index and an aspheric surface on the image side. Thus, even when the thickness at large light beam height of the object side negative lens element L1 is small so that the compensation of distortion or curvature of field on the wide-angle limit side is insufficient, in the entire zoom lens system according to Embodiment 3, the compensation effect of the image side positive lens element L2 allows the image side positive lens element L2 to compensate sufficiently the distortion and the curvature of field on the wide-angle limit side.
As shown in
In the zoom lens system according to Embodiment 4, the second lens unit G2, in order from the object side to the image side, comprises: a bi-convex third lens element L3; a bi-concave fourth lens element L4; a negative meniscus fifth lens element L5 with the convex surface facing the object side; and a bi-convex sixth lens element L6. Among these, the third lens element L3 and the fourth lens element L4 are cemented with each other and thereby constitute a positive cemented lens element, while the fifth lens element L5 and the sixth lens element L6 are cemented with each other and thereby constitute a positive cemented lens element. Further, the third lens element L3 serving as the most object side lens element of the second lens unit G2 has an aspheric object side surface.
In the zoom lens system according to Embodiment 4, the third lens unit G3 comprises solely a bi-convex seventh lens element L7. The seventh lens element L7 has an aspheric image side surface.
In the zoom lens system according to Embodiment 4, the two lens elements L1 and L2 constituting the first lens unit G1 contact with each other in a vicinity where the light beam from the object passes. Thus, the thickness of the entire first lens unit G1 can be reduced. Further, even when the object side negative lens element L1 and the image side positive lens element L2 of the first lens unit G1 approach with each other so that the capability of compensating distortion is degraded, the distortion at the wide-angle limit is compensated satisfactorily in the entire zoom lens system according to Embodiment 4 since the image side positive lens element L2 is a lens element having a comparatively high refractive index as shown in Table 16 described later, and an aspheric surface on the image side.
As shown in
Further, in the zoom lens system according to Embodiment 5, the second lens unit G2, in order from the object side to the image side, comprises: a bi-convex third lens element L3; a bi-concave fourth lens element L4; and a bi-convex fifth lens element L5. Among these, the third lens element L3 and the fourth lens element L4 are cemented with each other and thereby constitute a positive cemented lens element. Further, the third lens element L3 serving as the most object side lens element of the second lens unit G2 has an aspheric object side surface.
Further, in the zoom lens system according to Embodiment 5, the third lens unit G3 comprises solely a positive meniscus sixth lens element L6 with the convex surface facing the image side. The sixth lens element L6 has an aspheric object side surface and an aspheric image side surface.
In the zoom lens system according to Embodiment 5, as shown in Table 16 described later, the image side positive lens element L2 constituting the first lens unit G1 has a notably high refractive index. Thus, in the object side negative lens element L1, the thickness at large light beam height is easily ensured, so that the lens thickness can be reduced. Thus, in the zoom lens system according to Embodiment 5, the overall optical length at the time of non-use is reduced.
In the zoom lens system according to Embodiments 1 to 5, the lens units G1 to G3 are arranged in a desired optical power construction so that size reduction is achieved in the entire lens system in a state that excellent optical performance is satisfied.
In particular, in the zoom lens system according to Embodiments 1 to 5, the first lens unit G1 is constructed from: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side. Further, the second lens unit G2 is constructed from two sets of positive cemented lens elements each fabricated by cementing two lens elements, or alternatively has such a construction that one set of cemented lens element is placed between positive lens elements each arranged on the object side or the image side. Furthermore, the third lens unit G3 is constructed from one lens element. As such, the zoom lens system according to Embodiments 1 to 5 realizes a lens system that has a small number of lens elements constituting each lens unit and a short overall optical length at the time of non-use.
As described above, in the zoom lens system according to Embodiments 1 to 5, the second lens unit G2 is constructed from two sets of positive cemented lens elements or alternatively has such a construction that one set of cemented lens element is placed between positive lens elements each arranged on the object side or the image side. Instead, the second lens unit G2 may, in order from the object side to the image side, comprise one set of positive cemented lens element and one positive lens element, so that a lens system can be realized that has a short overall optical length at the time of non-use.
In the zoom lens system according to Embodiments 1 to 5, each of the object side negative lens element and the image side positive lens element constituting the first lens unit G1 has an aspheric surface, while the image side positive lens element has a specific refractive index and a specific Abbe number. Thus, the zoom lens system according to Embodiments 1 to 5 has excellent optical performance, for example, in compensation of curvature of field.
Conditions are described below that are to be satisfied by a zoom lens system like the zoom lens system according to Embodiments 1 to 5, in order from the object side to the image side, comprises a first lens unit having negative optical power, a second lens unit having positive optical power, and a third lens unit having positive optical power, wherein the first lens unit is constructed from: one object side negative lens element with the convex surface facing the object side; and one image side positive lens element with the convex surface facing the object side, and wherein each of the two lens elements constituting the first lens unit has an aspheric surface. Here, a plurality of conditions to be satisfied are set forth for the zoom lens system according to each embodiment. The construction that satisfies all the conditions is most desirable for the zoom lens system. However, when an individual condition is satisfied, a zoom lens system providing the corresponding effect can be obtained.
For example, in a zoom lens system like the zoom lens system according to Embodiments 1 to 5, the following conditions (1), (2) and (3) are satisfied;
n12>1.88 (1)
v12<26 (2)
5.0<αiW<20.0 (3)
(here, ωW>30)
where,
n12 is a refractive index of the image side positive lens element of the first lens unit,
v12 is an Abbe number of the image side positive lens element of the first lens unit,
αiW is an incident angle of the principal ray onto the image sensor at the maximum image height at a wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is a half view angle at a wide-angle limit.
The conditions (1) and (2) set forth the refractive index and the Abbe number of the image side positive lens element constituting the first lens unit. When these conditions (1) and (2) are satisfied, the center thickness of the image side positive lens element becomes small, while curvature of field on the wide-angle limit side is suppressed without the necessity of a large curvature in the image side surface, so that edge thickness is easily ensured. Thus, the thickness of the first lens unit can be reduced. This reduces the thickness of the entire zoom lens system and hence the overall optical length at the time of non-use.
The condition (3) sets forth the incident angle of the principal ray onto the image sensor at the maximum image height at the wide-angle limit. When the condition (3) is satisfied, the incident angle of the most off-axial principal ray that is incident onto the image sensor becomes small. This reduces the influence of shading. When the value exceeds the upper limit of the condition (3), a possibility arises that the influence of shading of the image sensor causes a decrease in the amount of periphery light. In contrast, when the value goes below the lower limit of the condition (3), the negative angle of the most off-axial principal ray at the telephoto limit becomes large at the time of magnification change. This causes a possibility that the amount of periphery light is reduced especially at the telephoto limit.
Here, when at least one of the following conditions (1)′ and (2)′ is satisfied, the above effect is achieved more successfully. When the following condition (1)′ is satisfied, the image side positive lens element of the first lens unit can have a large Z value (difference between curvature of the object side surface and curvature of the image side surface), so that the centering of the lens becomes easier. Further, when the following condition (2)′ is satisfied, chromatic aberration generated in the first lens unit can be compensated more satisfactorily.
n12>1.95 (1)′
v12<24 (2)′
Further, when the following condition (3)′ is satisfied, fluctuation in the incident angle of the principal ray onto the image sensor at the maximum image height is suppressed in zooming and so is fluctuation in the amount of periphery light. Thus, this configuration is remarkably effective.
αiW<15.0 (3)′
Further, for example, in a zoom lens system like the zoom lens system according to Embodiments 1 to 5, it is preferable that the following conditions (4), (5), (6) and (7) are satisfied;
n11>1.50 (4)
v11>35 (5)
n12−n11>0.10 (6)
v11−v12>15.0 (7)
where,
n11 is a refractive index of the object side negative lens element of the first lens unit,
v11 is an Abbe number of the object side negative lens element of the first lens unit,
n12 is the refractive index of the image side positive lens element of the first lens unit, and
v12 is the Abbe number of the image side positive lens element of the first lens unit.
The conditions (4) and (5) set forth the refractive index and the Abbe number of the object side negative lens element constituting the first lens unit. The conditions (6) and (7) relate to conditions for performing satisfactory compensation of chromatic aberration of a zoom lens system where the first lens unit is of negative-lead and has negative optical power while the first lens unit comprises an object side negative lens element and an image side positive lens element. When these conditions (4), (5), (6) and (7) are satisfied, a possibility is avoided that the optical axial thickness of the lens element increases with increasing light beam height and that when the center thickness is increased for the purpose of improvement in manufacturability, the thickness of the entire first lens unit increases further. At the same time, chromatic aberration can be compensated satisfactorily.
Further, when at least one of the following conditions (4)′, (5)′, (6)′ and (7)′ is satisfied, the above effect is achieved more successfully. Furthermore, when at least one of the following conditions (5)″ and (7)″ is satisfied, chromatic aberration generated in the first lens unit can be compensated more satisfactorily.
n11>1.75 (4)′
v11>38 (5)′
65>v11 (5)″
n12−n11>0.12 (6)′
v11−v12>17.5 (7)′
45.0>v11−v12 (7)″
Further, for example, in a zoom lens system like the zoom lens system according to Embodiments 1 to 5, it is preferable that the following condition (8) is satisfied;
T1/Y<1.5 (8)
where,
T1 is a center thickness of the first lens unit, and
Y is the maximum image height.
The condition (8) sets forth the center thickness of the first lens unit in a zoom lens system where the first lens unit is of negative-lead and has negative optical power, and hence easily becomes large. When the condition (8) is satisfied, a possibility is avoided that the thickness of the first lens unit increases excessively and so does the overall optical length at the time of non-use.
Further, when the following condition (8)′ is satisfied, optical power is imparted to the air lens in the first lens unit. Thus, the compensation of curvature of field becomes easier on the wide-angle side.
0.8<T1/Y (8)′
Further, for example, in a zoom lens system like the zoom lens system according to Embodiments 1 to 5, it is preferable that the following condition (9) is satisfied;
(T1+T2+T3)/Y<3.5 (9)
where,
T1 is the center thickness of the first lens unit,
T2 is a center thickness of the second lens unit,
T3 is a center thickness of the third lens unit, and
Y is the maximum image height.
The condition (9) sets forth the total center thickness of the lens units. When the condition (9) is satisfied, a possibility is avoided that the total thickness of the lens units increases excessively and so does the overall optical length at the time of non-use.
When the following condition (9)′ is satisfied, the above effect is achieved more successfully. Further, when the following condition (9)″ is satisfied, the thickness of each lens unit, especially the thickness of the first lens unit and the thickness of the second lens unit, can be ensured. This permits more satisfactory compensation of curvature of field.
(T1+T2+T3)/Y<3.2 (9)′
2.5<(T1+T2+T3)/Y (9)″
Further, for example, in a zoom lens system like the zoom lens system according to Embodiments 1 to 5, it is preferable that the following condition (10) is satisfied;
3.0<f3/fW<5.5 (10)
(here, ωW>30)
where,
f3 is a composite focal length of the third lens unit,
fW is a focal length of the entire zoom lens system at a wide-angle limit, and
ωW is the half view angle at the wide-angle limit.
The condition (10) sets forth an appropriate focal length of the third lens unit. When the value goes below the lower limit of the condition (10), the necessary optical power of the third lens unit becomes large. This causes a difficulty in compensation of spherical aberration or coma aberration in a variable magnification range where the third lens unit comparatively approaches the object side. In contrast, when the value exceeds the upper limit of the condition (10), the necessary optical power of the third lens unit becomes small. This causes an increase in the amount of movement of the third lens unit, and hence causes difficulty in size reduction of the optical system.
Here, when at least one of the following conditions (10)′ and (10)″ is satisfied, the above effect is achieved more successfully.
3.8<f3/fW (10)′
f3/fW<4.4 (10)″
Further, for example, in a zoom lens system like the zoom lens system according to Embodiments 1 to 5, it is preferable that the following condition (11) is satisfied;
|αW−αiT|<15.0 (11)
(here, ωW>30)
where,
αiW is the incident angle of the principal ray onto the image sensor at the maximum image height at the wide-angle limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis),
αiT is an incident angle of the principal ray onto the image sensor at the maximum image height at a telephoto limit (here, the incident angle is defined as positive when the principal ray is incident on the light receiving surface of the image sensor with departing from the optical axis), and
ωW is the half view angle at the wide-angle limit.
The condition (11) sets forth the incident angle of the principal ray onto the image sensor at the maximum image height at the time of zooming. When the condition (11) is satisfied, fluctuation in the incident angle of the most off-axial principal ray that is incident onto the image sensor becomes small, so that fluctuation in the seeing condition of the image of the periphery part is maintained within an allowable range.
Here, when the conditions (3) and (11) are satisfied simultaneously, the illuminance of image periphery can be maintained appropriately. Thus, this configuration is remarkably preferable.
Here, the lens units constituting the zoom lens system of Embodiments 1 to 5 are composed exclusively of refractive type lens elements that deflect the incident light by refraction (that is, lens elements of a type in which deflection is achieved at the interface between media each having a distinct refractive index). However, the present invention is not limited to the zoom lens system of this construction. For example, the lens units may employ diffractive type lens elements that deflect the incident light by diffraction; refractive-diffractive hybrid type lens elements that deflect the incident light by a combination of diffraction and refraction; or gradient index type lens elements that deflect the incident light by distribution of refractive index in the medium.
Further, in the zoom lens system according to Embodiments 1 to 5, when a reflecting surface may be arranged in the optical path so that the optical path may be bent before or after the zoom lens system or alternatively in the middle. The bending position may be set up arbitrarily depending on the necessity. When the optical path is bent appropriately, thickness reduction in appearance can be achieved in a camera.
As described above, according to the present invention, a zoom lens system is obtained that compensates curvature of field satisfactorily and that still has a reduced thickness of the first lens unit and a short overall optical length at the time of non-use.
The lens barrel comprises a main barrel 5, a moving barrel 6, and a cylindrical cam 7. When the cylindrical cam 7 is rotated, the first lens unit G1, the second lens unit G2, and the third lens unit G3 move to predetermined positions relative to the image sensor 2, so that variable magnification can be achieved ranging from the wide-angle limit to the telephoto limit. The third lens unit G3 is movable in the optical axis direction by a motor for focus adjustment.
As such, when the zoom lens system according to Embodiment 1 is employed in a digital still camera, a small digital still camera is obtained that has a high resolution and high capability of compensating the curvature of field and that has a short overall optical length at the time of non-use. Here, in the digital still camera shown in
An imaging device comprising a zoom lens system according to Embodiments 1 to 5 described above and an image sensor such as a CCD or a CMOS may be applied to a mobile telephone, a PDA (Personal Digital Assistance), a surveillance camera in a surveillance system, a Web camera, a vehicle-mounted camera or the like.
Hereinafter, numerical examples which are actual implementations of the zoom lens systems according to Embodiments 1 to 5 will be described. In the numerical examples, the units of the length in the tables are all “mm”. The units of the angle in the tables are all “degree”. Moreover, r is the radius of curvature, d is the axial distance, nd is the refractive index to the d-line, and vd is the Abbe number to the d-line. In the numerical examples, the surfaces marked with * are aspherical surfaces, and the sag z of the aspherical surface is defined by the following expression:
Here, h is the height from the optical axis, c is the curvature, k is the conic constant, and A, B, C, D and E are the fourth-order, sixth-order, eighth-order, tenth-order and twelfth-order aspherical coefficients, respectively.
A zoom lens system of Example 1 corresponds to Embodiment 1 shown in
TABLE 1
Lens
Lens unit
element
Surface
r
d
nd
νd
G1
L1
1
51.824
1.100
1.805
41.0
*2
6.287
2.433
L2
3
12.887
1.400
2.400
17.0
*4
17.651
Variable
Diaphragm
5
∞
0.300
G2
L3
*6
4.617
1.900
1.805
41.0
L4
7
30.191
0.500
1.717
29.5
8
4.069
0.600
L5
9
19.289
0.600
1.620
36.3
L6
10
4.413
1.200
1.589
61.3
11
−12.764
Variable
G3
L7
12
−237.873
1.100
1.665
55.2
*13
−15.297
Variable
P
14
∞
0.900
1.517
64.2
15
∞
0.870
TABLE 2
Surface
k
A
B
C
D
E
2
−3.612E−01
7.170E−06
−3.185E−06
−1.903E−09
−1.340E−09
0.000E+00
4
0.000E+00
−9.258E−05
1.154E−06
0.000E+00
0.000E+00
0.000E+00
6
0.000E+00
−5.397E−04
−1.839E−05
1.169E−07
−3.148E−08
0.000E+00
13
0.000E+00
4.422E−04
−5.274E−05
6.216E−06
−3.426E−07
7.090E−09
TABLE 3
Axial
Wide-angle
Middle
Telephoto
distance
limit
position
limit
d4
14.79
8.07
2.37
d11
2.70
9.09
19.06
d13
6.10
4.47
2.64
f
5.36
8.81
16.71
F-number
2.98
3.86
5.66
2ω
70.01
44.60
23.97
L
36.50
34.53
36.96
A zoom lens system of Example 2 corresponds to Embodiment 2 shown in
TABLE 4
Lens
Lens unit
element
Surface
r
d
nd
νd
G1
L1
1
97.238
1.300
1.878
38.2
*2
6.116
2.181
L2
3
15.696
1.778
1.996
20.5
*4
62.842
Variable
Diaphragm
5
∞
0.300
G2
L3
*6
4.711
1.500
1.804
40.8
7
20.931
0.300
L4
8
8.092
0.800
1.697
55.5
L5
9
52.433
0.400
1.805
25.5
10
3.521
0.419
L6
11
24.775
0.993
1.697
55.5
12
−24.775
Variable
G3
L7
13
33.551
1.438
1.518
70.3
*14
−15.270
Variable
P
15
∞
0.900
1.517
64.2
16
∞
0.870
TABLE 5
Surface
k
A
B
C
D
E
2
−7.285E−01
1.632E−04
−1.177E−05
3.548E−07
−1.538E−09
0.000E+00
4
0.000E+00
−1.619E−04
7.984E−06
−2.917E−07
2.109E−09
0.000E+00
6
−1.425E−01
−4.078E−04
1.138E−05
−7.290E−06
7.546E−07
0.000E+00
14
0.000E+00
2.119E−04
−1.102E−05
1.904E−07
1.254E−08
−4.126E−10
TABLE 6
Axial
Wide-angle
Middle
Telephoto
distance
limit
position
limit
d4
16.24
6.86
1.68
d12
2.70
7.90
17.30
d14
4.39
3.93
2.60
f
4.83
8.79
16.50
F-number
2.99
3.96
5.91
2ω
75.75
45.08
24.67
L
36.58
31.92
34.84
A zoom lens system of Example 3 corresponds to Embodiment 3 shown in
TABLE 7
Lens
Lens unit
element
Surface
r
d
nd
νd
G1
L1
1
−84.423
1.100
1.514
63.3
*2
5.404
2.309
L2
3
14.387
1.600
1.900
24.0
*4
26.719
Variable
Diaphragm
5
∞
0.300
G2
L3
*6
4.964
1.900
1.805
41.0
L4
7
144.593
0.500
1.717
29.5
8
4.496
0.600
L5
9
43.557
0.600
1.620
36.3
L6
10
6.034
1.200
1.589
61.3
11
−10.835
Variable
G3
L7
12
−237.873
1.100
1.665
55.2
*13
−14.202
Variable
P
14
∞
0.900
1.517
64.2
15
∞
0.870
TABLE 8
Surface
k
A
B
C
D
E
2
−6.222E−01
2.697E−04
−9.608E−06
−1.996E−07
4.805E−09
0.000E+00
4
0.000E+00
−2.732E−04
9.958E−06
−1.370E−07
0.000E+00
0.000E+00
6
0.000E+00
−5.198E−04
−1.810E−05
1.721E−06
−1.330E−07
0.000E+00
13
0.000E+00
4.072E−04
−5.130E−05
6.943E−06
−4.141E−07
9.128E−09
TABLE 9
Axial
Wide-angle
Middle
Telephoto
distance
limit
position
limit
d4
14.38
8.04
2.03
d11
2.70
9.14
19.40
d13
6.45
4.83
2.60
f
5.57
8.82
16.70
F-number
2.94
3.77
5.56
2ω
67.94
43.94
23.71
L
35.61
34.10
36.11
A zoom lens system of Example 4 corresponds to Embodiment 4 shown in
TABLE 10
Lens
Lens unit
element
Surface
r
d
nd
νd
G1
L1
1
96.707
1.100
1.878
38.2
*2
5.757
1.219
L2
3
9.382
1.778
1.996
20.5
*4
22.204
Variable
Diaphragm
5
∞
0.300
G2
L3
*6
4.225
1.500
1.805
41.0
L4
7
−50.000
0.600
1.717
29.5
8
3.642
0.600
L5
9
15.017
0.600
1.620
36.3
L6
10
5.586
1.500
1.589
61.3
11
−16.364
Variable
G3
L7
12
100.000
1.100
1.665
55.2
*13
−15.520
Variable
P
14
∞
0.900
1.517
64.2
15
∞
0.870
TABLE 11
Surface
k
A
B
C
D
E
2
−7.802E−01
5.551E−05
1.727E−07
−1.998E−07
6.955E−09
0.000E+00
4
0.000E+00
−4.846E−05
3.420E−06
4.006E−08
−4.178E−09
0.000E+00
6
0.000E+00
−6.412E−04
−4.796E−05
6.036E−06
−6.470E−07
0.000E+00
13
0.000E+00
7.442E−04
−9.347E−05
9.894E−06
−5.255E−07
1.088E−08
TABLE 12
Axial
Wide-angle
Middle
Telephoto
distance
limit
position
limit
d4
16.77
7.10
2.17
d11
2.70
8.24
17.94
d13
4.97
4.43
2.64
f
4.75
8.81
16.43
F-number
2.78
3.66
5.40
2ω
76.50
44.06
24.09
L
36.51
31.84
34.82
A zoom lens system of Example 5 corresponds to Embodiment 5 shown in
TABLE 13
Lens
Lens unit
element
Surface
r
d
nd
νd
G1
L1
1
219.620
1.300
1.665
55.2
*2
5.394
1.332
L2
3
10.390
1.700
1.923
20.9
*4
19.494
Variable
Diaphragm
5
∞
0.300
G2
L3
*6
4.332
1.969
1.805
41.0
L4
7
−24.440
0.500
1.755
27.5
8
3.693
0.582
L5
9
10.572
1.100
1.487
70.4
10
−13.751
Variable
G3
L6
*11
−268.064
1.400
1.750
45.4
*12
−13.878
Variable
P
13
∞
0.900
1.517
64.2
14
∞
0.870
TABLE 14
Surface
k
A
B
C
D
E
2
−5.814E−01
2.649E−05
−1.759E−05
1.597E−07
3.392E−09
0.000E+00
4
0.000E+00
−1.373E−04
1.587E−05
−3.585E−07
1.163E−10
0.000E+00
6
0.000E+00
−5.954E−04
−1.623E−05
−2.576E−06
2.704E−07
0.000E+00
11
0.000E+00
−1.834E−04
−4.044E−05
2.363E−07
−1.862E−08
0.000E+00
12
0.000E+00
6.049E−05
−2.992E−05
−3.988E−07
3.768E−09
0.000E+00
TABLE 15
Axial
Wide-angle
Middle
Telephoto
distance
limit
position
limit
d4
16.49
6.45
2.35
d10
2.70
7.00
17.78
d12
4.78
5.08
2.60
f
4.74
8.79
16.54
F-number
2.92
3.75
5.76
2ω
77.10
44.80
24.10
L
35.92
30.48
34.69
Table 16 shows values corresponding to the conditions in Examples 1 to 5.
TABLE 16
Example
Condition
1
2
3
4
5
(1)
n12
2.40
2.00
1.90
2.00
1.92
(2)
ν12
17.0
20.5
24.0
20.5
20.9
(3)
αiW
12.0
12.5
10.3
8.8
10.0
(4)
n11
1.81
1.88
1.51
1.88
1.67
(5)
ν11
41.0
38.2
63.3
38.2
55.2
(6)
n12 − n11
0.60
0.12
0.39
0.12
0.26
(7)
ν11 − ν12
24.0
17.7
39.3
17.7
34.3
(8)
T1/Y
1.37
1.46
1.39
1.14
1.20
(9)
(T1 + T2 + T3)/Y
3.01
3.09
3.03
2.78
2.75
(10)
f3/fW
4.6
4.2
4.1
4.3
4.1
(11)
|αiW − αiT|
10.2
12.3
9.2
7.7
9.5
T1
4.93
5.26
5.01
4.10
4.33
T2
4.80
4.41
4.80
4.80
4.15
T3
1.10
1.44
1.10
1.10
1.40
T1 + T2 + T3
10.83
11.11
10.91
10.00
9.88
Y
3.60
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The zoom lens system according to the present invention is applicable to a camera such as a digital still camera, a digital video camera, a mobile telephone, a PDA (Personal Digital Assistance), a surveillance camera in a surveillance system, a Web camera or a vehicle-mounted camera. In particular, the present zoom lens system is suitable for a camera such as a digital still camera or a digital video camera requiring high image quality.
Although the present invention has been fully described by way of example with reference to the accompanying drawings, it is to be understood that various changes and modifications will be apparent to those skilled in the art. Therefore, unless otherwise such changes and modifications depart from the scope of the present invention, they should be construed as being included therein.
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| Feb 09 2007 | KURIOKA, YOSHIAKI | MATSUSHITA ELECTRIC INDUSTRIAL CO , LTD | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 019853 | /0831 | |
| Mar 01 2007 | Panasonic Corporation | (assignment on the face of the patent) | / | |||
| Oct 01 2008 | MATSUSHITA ELECTRIC INDUSTRIAL CO , LTD | Panasonic Corporation | CHANGE OF NAME SEE DOCUMENT FOR DETAILS | 021897 | /0588 | |
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